-r (~~v A REPORT OF THE FACTORS ACCURACY submitted AN ON to the INVESTIGATION AFFECTING BUBBLE OF THE METERS Secretary of the Faculty as a partial fulfillment of the requirements for the degree of Bachelor submitted by of Science g--June 1, 1922. - I wish to take this opportunity to express my thanks to Professor R. T. Wilson, who suggested the investigation, Mr. G. R. Taylor who offered many and also to valuable suggestions during the course of the investigation. June 1, 1922 Signed. Table of Contents Introduction-------------------Page 1 Types of Flow Meters------------" 1 Factors Involved----------------" 3 Apparatus------------------" 6 Plate 1 ------------------------ " 8 Details of the Investigation--" 9 Plate 2 ------------------------ " 11 3 ----------------------- "12 4 ----------------------- "13 5 ----------------------- "14 6 ------------------------ " 15 7 ----------------------- "17 8------------------------ "18 "t 9------------------------ "20 10 ----------------------- "-21 11 ------------------------- "22 12 ----------------------- "23 Future Work-------------------" 24 25 Conclusions-------------------- " Data Sheets-+----------------- "26 130535 A. Introduction In experimental work of a chemical nature the reactions of gases play a very important part. Due to the comparatively large spaces between the molecules of gases, and due also to the rapid rates of diffusion, gases mix both rapidly and completely, the accompanying reactions being frequently the cause of heat evolution. The evolution of heat often passels unnoticed in laboratory experiments but almost always must be considered in.reactions that are to be carried on under industrial conditions. Complete control of exothermic reactions is,therefore, an absolute necessity because of the cumulative effect of heat liberThere are also many other types of gas ation. reactions used in laboratory practice which must be under complete control in order to As an accurate knowledge of insure safety. fact must precede regulation of any kind, so, before regulating the flow of a gas, its rate of flow must be known and a flow meter of some kind must be used. B. Types of Flow Meters The flow meters available for the measurement of the flow of fluids, whmle entirely satisfactory for many things, still leave a great It can readily be seen that deal to be desired. a prime requirement for a meter, to measure gases in the laboratory, is the ability to measure low If such a meter velocities and small volumes. can be made, that will also have the ability to withstand corrosion, the advantages to be obtained Two of the by its use are greatly increased. .2 most common and reliable types of instruments are Wide as is the Pit~t tubes and Venturi meters. field of these meters it does not include that of the measurement of low velocities; in fact the minimum velocitie-s which such instruments will measure has been placed by Bentoni at 1.75 cubic Displacement meters, although feet per minute. very accurate, do not give direct readings of volumes but a reading which must have a correctThis type of meter also has anion applied. other very serious disadvantage, that is that it is not of the continuous action type and must be placed at one or the other ends of the apparAnemometers are expensive, easily corroded, atus. Orifices can and inaccurate at low velocities. be made in glass and will not be corroded, but as the small hole necessitated by low velocities is not only very hard to make, but also requires very careful calibration, the use of such a meter Resistance tube entails certain disadvantages. meters, which depend on the friction drop in pressure over a length of pipe, are good instruments for the measurement of small volumes, but also require careful calibration The most common type of flow-meter for laboratory use is the capillary tube meter, a combination of the orifice and resistance tube It consists of a tubeabout three types. quarters of an inch in diameter, which is connected to the arms of a plain or multiplying differential guage and having a piece of capillary tubing , passing through a rubber stopper, placed between the guage, connections in the large This type of flow meter gives excellent tube.. results for small volumes but the capillary frequently becomes plugged and the meter like many others requires careful calibration. Calibration of meters for small volumes consists of passing air through the meter being calibrated and also through a mechanical meter in series with it, but as mechanical meters have a large percentage of error in measuring small volumes, the percentage error in measurements made by the calibrated meter will also be high. A bubble-meter, the possibilities of which I propose to investigate, will allow the gas flowing to bubble througha layer of liqutd which, of course, must be inert with respect to The volume the gas flowing through the meter. of gas passing through the meter will be equal to the number of bubbles multiplied by a constant. The determination of this constant for various conditions of meter operation is the problem of this investigation. C. Factors Involved The factors which will cause variations in the operation of the bubble-meter and which therefore must be investigated by passing air through the meter and noting the volume-number relations are: 1. The meter liquid. a. Water. b. Varied concentrations of sulphuric acid. c. Effect of impurities. I.' Soap. 2.1 Oil. 4 2. 3. The exit tip. a. Size. b. Type. The liquid head. The liquid to be used in the meter must This requirement be inert to the gas flowing. can be practically fullfilled by many different Water however liquids, chief of which is water. does keep many gasets in solution, but as thesaturation point of the meter liquid would be quickly reached, this disadvantage is of slight account. Water does have another disadvantage, namely, that it would humidify the air passing through the Sulphuric acid has many advantages over meter. water as a meter liquid chief of which are inactivity towards most gases and low vapor pressure with the resultant low magnitude of evaporation Hydrogen sulphide, hydrogen bromide losses. and hydrogen iodide will react with sulphuric acid at the temperatures at which such a meter would be used, consequently their measurement with sulphuric acid as a meter liquid is impossible. The effect of changing the concentration of the meter liquid will be to change the specific gravity and also the surface tension. Of these two factors the second is very important Another effect of as will be shown later. changing the concentration will be to change the Of course moisture content of the gas flowing. by choosing a suitable concentration to be used the moisture content of the exit gases can be kept where desired. 5 The size of the exit tUbp is important as it determines the size of the bubble to ascend through the liquid and consequently the number per unit volume of gas. The effect of changing the depth of the liquid will be to change the size of the bubbles and also, for a constant gas pressure to change the volume of gas to pass through the meter. The "Law of Tate" which states that the weight of a drop, 'W, is proportional to 2frr~ where r is the radius of the dropping tip andY~ is the surface tension of the liquid, has been proven .approximately true by Harkins 2 . He has shown that the weight of a drop is determined not only by the factors mentioned but also by the shape of the drop while forming. This shape factor is, however, constant for a single dropping tip. In order to apply the law or a similar one to bubbles the weight term"W"Vould have to be replaced by the difference in weight of the bubble and the displaced liquid, which is to say by the bouyancy of the bubble, the other factors representing the "Law of Tate" being unchanged.. As this investigation was not unders taken for the purpose of determining the weight or accurate volume. of a bubble, but rather to study bubbles of constant volume, reference has been made to the !Law of Tate" and the work of Harkins only to determitne the factors which will cause a change in the volume. of a bubble.For a given set of conditions within the meter the bubbles are of constant volume and the volume of gas to be measured is the product of the number of bubbles and the volume of one bubble. If the rate of flow is uniform the fact that some bubbles 6 are disengaged from the end of the tube before they have attained full growth will not interfere with the measurement of volume by this method as the bubbles will still be of constant volume for any definite velocity. D. Apparatus The apparatus used in this investigation is sketched diagrammatically in Plate 1 Air to which the following letters refer. ffom the laboratory pipe line was passed through an Allihn gas wash bottle "A" which contained the same kind and concentration of liquid as was Between in bottle "B", a Bunsen wash bottle. bottles "A" and "B" was placed a glass tee and two pinch cocks, one( of the screw type and one The branch of the of the spring pinch type. tee was connected to the first of two similar By regulating Bunsen bottles containing water. the screw clamp "H", the amount of air passing through bottle "B" could be controlled and the excess air would be diverefed through bottles By keeping the ratio of air passing "C" and "D".through bottles "C" and "D",to that passing through bottle "B", high, the effects of a varThe backiation of air pressure are minimized. pressure was kept constant by means of the arrangeA small ment shown at the bottom of Alate 1. pan "G" was placed inside the larger pan "F"; in the smaller pan was a glass tube fastened to a board,, on which graduate "E" was placed, with the end of the tube level with the top of the pan; as this pan was always full of water the back;pressure on bottle "B" was constant and always equal to atmospheric pressure plus the pressure necessary to U 7 overcome the friction in the rubber hose leadfrom bottle "B" to pan "G". The larger pan served merely to catch the water which continuously overflowed from pan "G". The volume of air measured by the graduate, being under less than atmospheric pressure, should be corrected but as this correction at its maximum is less than four percent, and very seldom that, it has been neglected in many cases, only being applied for the displacement of water near the top of the graduate. U-i ~1~ DETAILS I OF THE INVESTIGATION. 9 Of the factors which could cause a variation in the volume of a bubble, the first investigated was the size and type of tip used. Tips of different sizes were used in bottle "B", hereinafter refered to as the meter. The volume number relation is shown in Plates 2,3,4 andt5, from a comparison of which it can be seen that the inside diameter of the tube is the controilling factor and the outside diameter has little, if any,effect. The tube diameters were obtained by the use of micrometers and tapered pins; the internal diameters were measured by inserting tapered pins in the tubes and measuring with the micrometers the largest diameter that would enter The measurement of the outside diathe tube. meters was carried out zs a simple micrometer Measurements were made to three measurement. places, bat, owing to irregularity of the diameter of glass tubing, the third place is of doubtful value. Straight tips, horizontal tips with a ninety degree bend near the end and vertical tips with a bend of one hundred and eighty degrees were used but only the straight tips gave The horizontal tips satisfactory results. gave very closely controlled velocities of flow, but, owing to the fact that water entered the lower part of the tip and cut down its effective For differdiameter such tips were not used. ent rates of flow the effective tip diameters of such tips would be different, as they also would for different depths of meter liquid. Tips bent through one hundred and eighty degrees are very unsatisfactory as the meter liquid enters the tube and thus constantly varies the liquid head in the meter. The result of the variations of liquid head is that the bubbles flow in a pulsating manner, which not only destroys the conditions of equilibrium, but also makes it impossible to count the bubbles. A tip cut with a hot wire was used and proved unsatisfactory as the tube end was not perfectly flat and at every projection a secondary stream of bubbles formed. Tips that, after having the projections ground or filed off, were smoothed in the Bunsen flame and tips that were ground on a fine abrasive wheel or oil stone did not give any such troubles as did the plain cut Attention should be called to the method tip. used by Harkins 2 for grinding dropping tips. This method consists of filling the tip and also surrounding it with "Wood's metal" and after grinding tip, metal and all of removing the metal by dipping the tip in hot water. To determine the effect of changing the liquid head on the operation of the meter, two runs were made, in one of which the liquid depth was one inch and in the other of which it was six and one quarter inches.- The results of these two runs are plotted, see Plate 8, and seem to show that the volume number relation is not appreciably changed by a slight change in the The effect of a height of the meter liquid. change in liquid head can, however, be put to a good use, as by changing the depth of the tip without changing the setting of screw clamp "H" the rate of flow is varied and thus control of the meter can be obtained. 12 C) cc:~ eARATCf L<Ca lit T - -l 14 li - 11 -- TH 41 1 4 Tf Tor t $ - IP lit 1J I tH _n-$ ttt Plate 6 i LL tj !V j1 H - K R . 7- T- MAJ 1 QtR T 11 - al- -~-H -t- S 4L -L _t1 T +4 t 44 -7 - -- --- -: r~~ SECH - t 41 i 4 7_ - T I . 44 7v '11 - TR - y itI7 L - -I -A - io 1 1ik y td _ 7 ol -r T t 1 IF -Il, F- + 4- 111 -d T1 T (_1T14 'CC17 1~1PT #-Y +vt~lIt~h ' - LO Y7 RANCH .ca e - s o r h 1t4 _4 s The effect of impurities was studied by adding a known weight of "Ivory" soap to the meter liquid and making runs to obtain the data necessary for plotting the curve. The concentration of the soap solution was changed several time- and runs were made for each soap concentration. Too fewoooints were obtained to enable the curve for the original soap concentration to be plotted. The results of the other runs are plotted on plate 7 and show that for concentrated soap solutions the ratio of number to volume is increased. As the concentrations are diminished the curve falls nearer and nearer that When the obtained with water in the meter. concentration of soap is such that it can be seen care, there if the water is examined with a little is no appreciable change in the number volume ratio. By adding a small amount of oil tp the final soap concentration, 0.003 gms. per liter, and emulsifying the oil, data was obtained for This curve appears to show curve(M) on Plate 8. that an oil emulsion either has a higher surface tension than water, or else the emulsion has a Of the two possibilities density less than onet that of lowered density is undoubtedly the factor responsible for the lowering of number volume ratio. As most impurities lower the surface tension of water, their effect can be predicted to be the same as that produced by dissolving soap in the water. 1 -1 44t1 -- -t - WH 7~ 4 _7O II 1-1-7 --- 7 t -T-4- Lt I' L - tn- -E H 7 -, T4H T 1- Pat L -7 T 4 7 . ( -I a -lT- -H m T T 7 11ii TET Ar o F -- 7o 4 B 4 Y A t C A B 17 Plate q 19 The effect of different liquids in the meter was determined by making runs on water, on sulphuric acid , specific gravity 1.435, andOn sulphuric acid, specific gravity 1.295. The runs made on these liquids are plotted on Plates 9,. 10 and 11. Plate 10 shows a sharp change in slppe in curve (M) beyond which point the points vary wildly. ,Plate 11 shows the specific gravity of the acid plotted against the volume of air flowing when one hundred and twenty five bubbles per minute pass through the meter. No definite conclusions can be drawn from this plot due to its irregularity but possibly the irregularities can be ex.)lained by the fact that increased density and lessened surface tension in the sulphuric acid tend to act so as to effect the number volume ratio in different ways. All runs were made by opening pinch cock "I" and allowing air to flow through the The meter for one and sometimes two minutes. bubbles were counted on a tallying counter and In the difference in graduate readings noted. counting, attention should be focused on one point in the meter, in the runs made such a point Preliminary to making was the end of the tube. any runs the screw clamp "H" was opened wide and air allowed to bubble rapidly through the meter to saturate the meter liquid. T1 Plate9 t 4 12-, b FA - 77- u + 17 -i 1 T tt u -Tp-- I -4 - t ~CI -L t -+ -j(A~ - I{+ -- - -4 - ,&+- - (Ml - 1 (2 L -I-!&Th1jThi$ -1 L - x -~ T --- _ - - - - -t7 -4_ 1 p Vp I- -> H- g .9 ~N - i .it- - - , - rI- 7-t-- -~ -4T ~-7- - - -L -t H -L T -V - - -- I u-- 4 N ttil- I ra 4T 1 -- - - uA- -I 79 uU pu - A-- - -T - Cl r7e 44- - 4 -. n 4-4 - -H a - fr-H- Hi -- tj . .. . .. .. . .. . 1 -MM -TTT -4T T+it -i-fd ~vfrHfN ARTFH-it 44 - -4 -- - V 121 1s(,) 2.9C I t n 1~ -L 0r - i I. -L4 L9 e~ 4i-- -H 7 * t 71 Fdt -WITIF 4+4 C i T -t 1 - T h4-- L 77t, _Il 4'4 $ t 4'+ 1 L1 -1 ftI Plate Li -T ItF g 12 $$$+ I 1 14 4 * J L 1YiI ------- -'-44 ifT LI4I TEHN HA v 1EC:0 nr - YJ 3 RNC '-YC11 - G i -'I 23 24 Future Work. The inability to accurately measure volumes greater than two hundred cubic centimeters by means of apparatus similar to that used in this investigation seems to necessitate the improvement of such apparatus. To the end of so improveing the meter I would recommend that future investigators determine the extent to which an aspirator bottle,with a horizontal tip and a carefully maintained constant liquid head,could Also in order that be used as a bubble meter. a bubble meter be capable of more universal use I would also recommend that its possibilities for the measurement of a heavy gas such as chlorine be determined. Conclusions The use of a bubble-meter, as herein described, is possible if volumes of less than 200 cubic centimeters per minute are to be Several precautions must however be measured. taken; the tips must be smooth and approximately horizontal, the liquids must be saturated with the gas being measuredand rubber and not cork stoppers should be used in the metering bottle. The depth of the exit tip should not be more than six nor less than one inch below the liquid A bubble-meter should not be used to surface. measure gases other air or cases of nearly the same weight, as Nitrogen or Oxygen,until further A high investigation has been carried out. degree of accuracy can be expected if two or The highest more runs can be made to check. percentage error obtained from Plate 2 is 20% The but the average is slightly less than 5%. error of 20Z occurred at a velocity of 5 0.0. per minute and for such a small displacement the volume displaced cannot be measured closer Larger than 20% with the apparatus used. tubes cannot be effectively used in a bubblemeter as the volume-number plot would have too steep a slope to give any great accuracy. APPENDIX DATA SHEET tip number 1 1. dia. 0.167", 2 " " 3 "f " 4 " " 0. dia. 0.1253" 0.1226". 0.320", 0. 367", " 0(397" 0.410" 0. 456" Meter liquid is water unless otherwise stated. All volumes are in cubic centimeters. Tip no. Volume 4 5 3.(5 11 13 13 12 14 13 number 24. 5 26 20 60 65 65 63 80 65 1 volume number 16 80 15 80 22.. i5 104 101 21. f5 21. 5 108 20 105 109" 21 21 110 82 16 Tip no. volume 14 13 14 15 13 15 25, 25 29 number 74 72 76 75 72 81 132 131 150 2 Volume number volume number volume number 25 325 29 26 29 30 53 30 53 57 60 8 84 80 80 74 73 84 142 90 143 138 143 142 60 80 63 63 65 65 64 65 58 71 76 88 153 148 159 152 162 159 168 174 150 160 168 20 4 85 95 98 '10 5 105 1100 108 108 110 115 119 129 198 210 216 219 238 205 237 229 234 229 230 247 Tip no. Volume number 143 145 19 249 :245 44 volume 2 number volume number Tip no. 3 volume 12 12 24 24 31 33 41 41 42 13 10 8 number volume number volume number 22 21 44 46 61 61 75 75 17 10 59 63 69 72 70 70 77 78 115 115 27 27 99 105 113 117 118 124 128 131 165 175 120 123 1:28 126 125 125 237 235 166 175 179 183 192 187 240 246 29 17 13 Tip no-. 4 volume number 23 32 35 48 53 53 54 54 53 55 41 49 51 78 83 83 75 75. 84 88 va-lumes number volume number 56 56 55 58 58 63 60 60 70 80. 74 77 73 76 83 95 80 75 103 118 120 125 127 125 130 159 160 158 159 164 164 164 175 173 180 135 140 145 150 + Tip no. 4 Volume number volume number 150 160 175 185 190 195 205 225 230 230 230 135 190 195 230 245 245 250 250 285 285 285 290 297 295 300 226 234 236 241 241 245 280 242 254 257 Tip no. 494 202 216 214 211 223 230 222 227 216 4 is 45 101 102 165 170 235 50 50 30 30 number 67 135 140 198 204 225 75 67 39 40 254 252 the following runs unless otherwise stated. soap solution 0.,374 gms / liter. used in meter liquid is Volume 21 25 55 volume number 42 volume 50 55 number 82? 84 volume 150 143 nymber 201 199 82 meter liquid is soap solution 0.094 gms //liter. Volume number volume number volume 140 174 163 163 35 196, 209 207 193 46 35 120 150 140 95 48 180 186 178 123 90 45 45 30 35 number. 121 70 63 42 50 2q Meter liquid is Volume 170 180 65 65 number 214 216 volume 94 95 35 Volume number 35 35 53 56 51 number volume 25 25 35 Meter liquid is 35 soap solution 0.023 gms. / liter. 65 58 soap solution 0.011 gms. volume 80 80 130 number number 116 114 168 / liter. volume number. 133 171 Meter liquid is soap solution 0.006 gms / liter. Volume 170 175 178 170 number volume 200 190 210 193 33 96 95 11 Meter liquid is Volume number 80 75 98 97 78 109 74 80 40 47 101 119 number 1'19 127 125 147 volume volume 47 S22 62 114 123 1 17 115 62 165 number 70 227 148 158 151 151 210 145 33 11? 60 60 soap solution 0.003 gms. 82 / liter. volume 165 1590 170 220 215 number number. 195 136 202 227 213 30 Meter liquid is Volume 220 210 120 125 160 140 number 212 212 140 147 191 173 soap solution and oil. volume 155 190 155 140 155 75 Meter liquid is water, number volume number 181 241 174 164 192 102 75 100 100 105 50 50 104 134 129 134 72 75 depth is 6.25". Volume number volume number volume number 75 70 70 30 35 35 30 105 10 1 103 51 54 51 51 63 67 70 75 40 25 25 103 102 10 6 110 54 44 20 135 140 140 150 150 34 180 186 182 197 195 volume number Depth is Volume 75 80 78 32 number 112 114 114 47 vp~lume number 30 100 155 30 46 138 195 46 1.0". 160 160 194 196 Meter liquid is sulphuric acid unless otherwise stated specific gravity is 1.435 Tip no.- 4 volume number Volume number volume number 249 199 193 135 95 95 90 95 165 170 180 214 237 226 189 138 137 136 137 220 230 244 185 170 205 190 200 270 285 177 175 45 43 Tip no. Volume 150 175 180 185 170 220 220 220 85 90 90 number 236 228 234 238 227 243 249 245 120 175 179 volume 100 90 140 130 145 145 150 75 75 75 115 246 236 230 228 226 224 237 236 235 65 64 25 25 19 20 29 27 71 70 35 36 46 47 108 112 62 62 volume number 43 40 37 87 3 number 196 182 226 207 228 :232 231 156 151 152 211 135 140 60 65 60 60 31 30 12 12 2525 233 129 136 134 132 72 71 32 32 Tip no. 9 Volume number volume number volume number 27 23 85 40 36 29 102 103 4 24 90 40 133 233 140 50 156 5.15 6 23.,5 21.15 22 84 Volume number 34 34 9.(5 24 211 211 75 151 9 10 32 62 64 40 113 183 189 Tip no. i volume number 24 24 28 26 143 180 170 170 volume number 14 15 110 111 .7 55 54 specific gravity of sulphuria acid 1.1295 Volume number volume number volume 36 39 12 13 13 45 50 48 222 225 228 19 20 18 117 115 113 51 232 49 17 17 232 116 38 38 38 41 138 196 215 205 111 6 5S. 5 number 190 210 85 89 39 39 37..'5 Tip no. Volume 5.15 5.15 10 number 22 21.5 43 9. 15 37.15 9 37.15 volume 16 15 17 16 36 number 60 61 62 60 128 Tip no. Volume 190 195 120 120 60 50 number 2383 242 190 192 106 102 volume 53 2 34 64 73 126 131 number 126 205 214 285 260 3 number 100 82 153 90 90 41 156 153 85 36 42 volume volume 43 1.7.5 15 15 number 38 40 35.15 32.i5 11.5 27. 5 12.15 27.15 volume number 110o 190 97 97 190 115 135 231 223 Tip no. 4 Volume 15 16. (5 29.65 number 30.15 34.15 33 59 64 63 Its 97 34.15 Sulphuric aci d sp. volume 52 55 90 110 105 number 141 162 159 gr. 1.190 Volume 75 Number 126 Sulphuric acid sp. gr.- 1.089 Volume 88 Number 124 135 178 195 194 34 Bibliography (1) 1919 A.F.Benton. Rates of Flow. (2) 1919 pp. Gas Flow Meters for Small 623 - Harkins and Brown. J. I. E. Chem. 11. Determination of Surface Tension and the Weight of Falling Drops. J. A. C. S. 41, pp. 499 / 524.